2019
DOI: 10.1103/physrevx.9.011027
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Ferromagnetism and Conductivity in Atomically Thin SrRuO3

Abstract: Atomically thin ferromagnetic and conducting electron systems are highly desired for spintronics, because they can be controlled with both magnetic and electric fields. We present ðSrRuO 3 Þ 1 − ðSrTiO 3 Þ 5 superlattices and single-unit-cell-thick SrRuO 3 samples that are capped with SrTiO 3. We achieve samples of exceptional quality. In these samples, the electron systems comprise only a single RuO 2 plane. We observe conductivity down to 50 mK, a ferromagnetic state with a Curie temperature of 25 K, and sig… Show more

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Cited by 64 publications
(77 citation statements)
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References 54 publications
(75 reference statements)
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“…Physically, the difference in the phase shifts in Eqs. (14) and (15) comes from the difference in the Berry phases of quadratic and linear dispersions 76 .…”
Section: Methodsmentioning
confidence: 99%
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“…Physically, the difference in the phase shifts in Eqs. (14) and (15) comes from the difference in the Berry phases of quadratic and linear dispersions 76 .…”
Section: Methodsmentioning
confidence: 99%
“…Although Weyl fermions have been predicted to exist in various oxides [6][7][8] , evidence for their existence in oxide materials remains elusive [9][10][11] . SrRuO 3 , a 4d ferromagnetic metal often used as an epitaxial conducting layer in oxide heterostructures [12][13][14][15] , provides a promising opportunity to seek the existence of Weyl fermions in a magnetic material. State-of-the-art oxide thin film growth technologies, augmented by machine learning techniques, may allow access to such topological matter.…”
mentioning
confidence: 99%
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“…(b) Summary of measurement results for all techniques used, where "n", "n.m." and "y" stand for "no", "not measured" and "yes", respectively. [18,61]. Torque magnetometry measurements revealed no significant signal in the fully annealed sample.…”
Section: Torque Magnetometrymentioning
confidence: 94%
“…Recent years have seen intense interest in stabilizing and controlling magnetic ordering in two-dimensional (2D) systems (1)(2)(3)(4)(5)(6)(7)(8)(9), motivated by both the potential to unlock new fundamental physics and enable new high-density, low-power spintronic device paradigms. Engineering magnetic anisotropy (MA) in 2D systems plays a critical role in realizing these new functionalities but remains challenging because of the lack of accessible control parameters.…”
Section: Introductionmentioning
confidence: 99%